We would like to motivate the dependence of the CME on tilt by examining the consequence of a minimal model calculation. Following [1]}, [2]}, [3]}, we get that the equilibrium current in response to the applied magnetic field can be calculated by the following formula:
\(J_z &= -\frac{e^2B}{2\pi \hbar ^2} \int _{\Lambda }^{-\Lambda } \frac{dk_z}{2\pi } \frac{d}{dz} \left[ n E_0^{-} + \sum _{m=n}^{N_{max}} \sum _{\gamma = \pm } E_m^{-,\gamma } \right]\) 
